Epitaxial substrate for semiconductor device, semiconductor device, and process for producing epitaxial substrate for semiconductor device

ABSTRACT

Provided is an epitaxial substrate having excellent two-dimensional electron gas characteristics and reduced internal stress due to strains. A channel layer is formed of a first group III nitride represented by In x1 Al y1 Ga z1 N (x1+y1+z1=1) so as to have a composition in a range determined by x1=0 and 0≦y1≦0.3. A barrier layer is formed of a second group III nitride represented by In x2 Al y2 Ga z2 N (x2+y2+z2=1) so as to have a composition, in a ternary phase diagram with InN, AlN and GaN being vertices, in a range surrounded by five straight lines determined in accordance with the composition (AlN molar fraction) of the first group III nitride.

TECHNICAL FIELD

The present invention relates to an epitaxial substrate that has a multi-layer structure composed of a group III nitride semiconductor, and more particularly, to a multi-layer structured epitaxial substrate for electronic devices and a method of manufacturing the same.

BACKGROUND ART

Nitride semiconductors having high breakdown electric field and high saturation electron velocity have been attracting attention as the next generation of semiconductor materials for high-frequency/high-power devices. In particular, a multi-layer structure formed by laminating layers formed of AlGaN and GaN has the feature that high-concentration two-dimensional electron gas (2DEG) is generated at a lamination interface (hetero interface) owing to a large polarization effect (spontaneous polarization effect and piezo polarization effect) inherent in a nitride material, and hence a high electron mobility transistor (HEMT) using the multi-layer structure as a substrate has been developed vigorously (for example, see “Highly Reliable 250 W High Electron Mobility Transistor Power Amplifier”, Toshihide Kikkawa, Jpn. J. Appl. Phys. 44 (2005), p. 4896).

In order to put the above-mentioned HEMT device or a substrate for HEMT device that is a multi-layer structure used in manufacturing the same to practical use, various problems need to be solved: problems related to performance improvement such as increase of power density and efficiency, problems related to functional improvement such as achieving normally-off operation, and fundamental problems such as enhancing reliability and reducing cost. The above-mentioned problems are individually tackled vigorously.

For example, it is conceivable that controllable current density of a HEMT device, that is, power density capable of being utilized can be improved significantly if the concentration of two-dimensional electron gas existing in a substrate for HEMT device can be increased significantly. In a case of a nitride HEMT device having the most typical configuration in which a channel layer is formed of GaN and a barrier layer is formed of AlGaN, it is known that the concentration of two-dimensional electron gas increases along with an increase in AlN molar fraction of AlGaN that forms the barrier layer (for example, see “Gallium Nitride Based High Power Heterojunction Field Effect Transistors: Process Development and Present Status at USCB”, Stacia Keller, Yi-Feng Wu, Giacinta Parish, Naiqian Ziang, Jane J. Xu, Bernd P. Keller, Steven P. DenBans, and Umesh K. Mishra, IEEE Trans. Electron Devices 48 (2001), p. 552).

Further, growing attention is also paid to the HEMT device that has a low dependence on the piezo polarization effect, is capable of generating two-dimensional electron gas at high concentration almost only by spontaneous polarization, and has the structure with small strains, such as the HEMT device in which a channel layer is formed of GaN and a barrier layer is formed of InAlN (for example, see “Can InAlN/GaN be an alternative to high power/high temperature AlGaN/GaN devices?”, F. Medjdoub, J.-F. Carlin, M. Gonschorek, E. Feltin, M. A. Py, D. Ducatteau, C. Gaquiere, N. Grandjean, and E. Kohn, IEEE IEDM Tech. Digest in IEEE IEDM 2006, p. 673).

In a case of a HEMT device having an AlGaN/GaN heterostructure, when a barrier layer is formed of AlGaN having a large AlN molar fraction for increasing a two-dimensional electron gas concentration, a tensile stress generated inside the barrier layer increases. This leads to degradation in film quality and deterioration in surface form (such as increase of strains and occurrence of cracks). As a result, there occur various problems that “expected high two-dimensional electron gas concentration cannot be obtained (less than 2×10¹³/cm² at most)”, “various contact characteristics such as schottky and ohmic ones become deteriorated”, “unnecessary surface level is formed, which deteriorates device dynamic characteristics”, and the like.

Further, growing attention is paid to a laminated structure capable of obtaining higher two-dimensional electron gas concentration almost only by spontaneous polarization, as the InAlN/GaN heterostructure disclosed in Medjdoub et al. above. As to such laminated structure, for example, it is proposed to form a channel layer of GaN, form a barrier layer of In_(x)Al_(1-x)N (x: to 0.18) having a composition that is lattice-matched to an a-axis of GaN, and further faun a thin spacer layer of AlN between the channel layer and the barrier layer. However, the means for achieving the above in a specific manner and other effective configuration example are not expressly described because there is a large difference in growth temperature between InN and AlN, which makes it difficult to control epitaxial growth in a mixed crystal composition containing both.

DISCLOSURE OF INVENTION

The present invention has been made in view of the above-mentioned problems, and an object thereof is to provide an epitaxial substrate having excellent two-dimensional electron gas characteristics and reduced internal stress due to strains.

In order to solve the above-mentioned problems, according to a first aspect of the present invention, in an epitaxial substrate including: a base substrate; a channel layer formed of a first group III nitride containing at least Al and Ga and having a composition of In_(x1)Al_(y1)Ga_(z1)N (x1+y1+z1=1); and a barrier layer formed of a second group III nitride containing at least In and Al and having a composition of In_(x2)Al_(y2)Ga_(z2)N (x2+y2+z2=1), the composition of the first group III nitride is in a range determined by x1=0 and 0≦y1≦0.3; and the composition of the second group III nitride is, in a ternary phase diagram with InN, AlN and GaN being vertices, in a range surrounded by straight lines respectively represented by the following expressions determined in accordance with the composition of the first group III nitride.

$\begin{matrix} {{x\; 2} = {\frac{{y\; 2} - \left( {0.36 + {0.5y\; 1}} \right)}{1.78} = {- \frac{{z\; 2} - \left( {0.64 - {0.5y\; 1}} \right)}{2.78}}}} & \left\lbrack {{Formula}\mspace{14mu} 1} \right\rbrack \\ {{x\; 2} = {\frac{{y\; 2} - \left( {0.45 + {y\; 1}} \right)}{4.5} = {- \frac{{z\; 2} - \left( {0.55 - {y\; 1}} \right)}{5.5}}}} & \left\lbrack {{Formula}\mspace{14mu} 2} \right\rbrack \\ {{x\; 2} = {{- \frac{{y\; 2} - \left( {0.9 - {0.7y\; 1}} \right)}{4.5}} = \frac{{z\; 2} - \left( {0.1 + {0.7y\; 1}} \right)}{3.5}}} & \left\lbrack {{Formula}\mspace{14mu} 3} \right\rbrack \\ {{z\; 2} = 0} & \left\lbrack {{Formula}\mspace{14mu} 4} \right\rbrack \\ {{x\; 2} = {0\mspace{14mu} \left( {{{where}\mspace{14mu} \frac{9}{34}} \leq {y\; 1} \leq 0.3} \right)}} & \left\lbrack {{Formula}\mspace{14mu} 5} \right\rbrack \end{matrix}$

According to a second aspect of the present invention, in the epitaxial substrate for semiconductor device according to the first aspect, the composition of the second group III nitride is, in a ternary phase diagram with InN, AlN and GaN being vertices, in a range surrounded by straight lines respectively represented by the following expressions.

$\begin{matrix} {{x\; 2} = {\frac{{y\; 2} - \left( {0.5 + {0.5y\; 1}} \right)}{1.78} = {- \frac{{z\; 2} - \left( {0.5 - {0.5y\; 1}} \right)}{2.78}}}} & \left\lbrack {{Formula}\mspace{14mu} 6} \right\rbrack \\ {{x\; 2} = {\frac{{y\; 2} - \left( {0.45 + {y\; 1}} \right)}{4.5} = {- \frac{{z\; 2} - \left( {0.55 - {y\; 1}} \right)}{5.5}}}} & \left\lbrack {{Formula}\mspace{14mu} 7} \right\rbrack \\ {{x\; 2} = {{- \frac{{y\; 2} - \left( {0.9 - {0.7y\; 1}} \right)}{4.5}} = \frac{{z\; 2} - \left( {0.1 + {0.7y\; 1}} \right)}{3.5}}} & \left\lbrack {{Formula}\mspace{14mu} 8} \right\rbrack \\ {{z\; 2} = 0} & \left\lbrack {{Formula}\mspace{14mu} 9} \right\rbrack \\ {{x\; 2} = {0\mspace{14mu} \left( {{{where}\mspace{14mu} \frac{9}{34}} \leq {y\; 1} \leq 0.3} \right)}} & \left\lbrack {{Formula}\mspace{14mu} 10} \right\rbrack \end{matrix}$

According to a third aspect of the present invention, the epitaxial substrate for semiconductor device according to the first or second aspect further includes a spacer layer formed of a third group III nitride having a composition of In_(x3)Al_(y3)Ga_(z3)N (x3+y3+z3=1), the spacer layer being formed between the channel layer and the barrier layer, containing at least Al, and having larger bandgap energy compared with the barrier layer.

According to a fourth aspect of the present invention, in the epitaxial substrate for semiconductor device according to any one of the first to third aspects, the composition of the first group III nitride is in a range determined by x1=0 and 0<y1≦0.1.

According to a fifth aspect of the present invention, in the epitaxial substrate for semiconductor device according to any one of the first to third aspects, the composition of the first group III nitride is in a range determined by x1=0 and 0.1<y1≦0.3.

According to a sixth aspect of the present invention, in the epitaxial substrate for semiconductor device according to the third aspect, the composition of the third group III nitride is in a range determined by x3=0 and 0≦z3≦0.05.

According to a seventh aspect of the present invention, in the epitaxial substrate for semiconductor device according to the sixth aspect, the third group III nitride is AlN.

According to an eighth aspect of the present invention, in a semiconductor device, a source electrode, a drain electrode and a gate electrode are provided on the barrier layer of the epitaxial substrate for semiconductor device according to any one of the first to seventh aspects.

According to a ninth aspect of the present invention, a method of manufacturing an epitaxial substrate for semiconductor device includes: a channel layer forming step of epitaxially forming a channel layer formed of a first group III nitride on a base substrate, the first group III nitride containing at least Al and Ga and having a composition of In_(x1)Al_(y1)Ga_(z1)N (x1+y1+z1=1); and a barrier layer forming step of epitaxially forming a barrier layer formed of a second group III nitride on the channel layer, the second group III nitride containing at least In and Al and having a composition of In_(x2)Al_(y2)Ga_(z2)N (x2+y2+z2=1), wherein: the composition of the first group III nitride is selected in a range determined by x1=0 and 0≦y1≦0.3; and the composition of the second group III nitride is selected, in a ternary phase diagram with InN, AlN and GaN being vertices, in a range surrounded by straight lines respectively represented by the following expressions determined in accordance with the composition of the first group III nitride.

$\begin{matrix} {{x\; 2} = {\frac{{y\; 2} - \left( {0.36 + {0.5y\; 1}} \right)}{1.78} = {- \frac{{z\; 2} - \left( {0.64 - {0.5y\; 1}} \right)}{2.78}}}} & \left\lbrack {{Formula}\mspace{14mu} 11} \right\rbrack \\ {{x\; 2} = {\frac{{y\; 2} - \left( {0.45 + {y\; 1}} \right)}{4.5} = {- \frac{{z\; 2} - \left( {0.55 - {y\; 1}} \right)}{5.5}}}} & \left\lbrack {{Formula}\mspace{14mu} 12} \right\rbrack \\ {{x\; 2} = {{- \frac{{y\; 2} - \left( {0.9 - {0.7y\; 1}} \right)}{4.5}} = \frac{{z\; 2} - \left( {0.1 + {0.7y\; 1}} \right)}{3.5}}} & \left\lbrack {{Formula}\mspace{14mu} 13} \right\rbrack \\ {{z\; 2} = 0} & \left\lbrack {{Formula}\mspace{14mu} 14} \right\rbrack \\ {{x\; 2} = {0\mspace{14mu} \left( {{{where}\mspace{14mu} \frac{9}{34}} \leq {y\; 1} \leq 0.3} \right)}} & \left\lbrack {{Formula}\mspace{14mu} 15} \right\rbrack \end{matrix}$

According to a tenth aspect of the present invention, in the method of manufacturing an epitaxial substrate for semiconductor device according to the ninth aspect, a temperature T1(° C.) for forming the channel layer is determined in a range where 950° C.≦T1<1,250° C.; and a temperature T2(° C.) for forming the barrier layer is determined in a range determined in accordance with a molar fraction x2 of InN of the second group III nitride, the range satisfying 800-667·x2(° C.)≦T2≦860-667·x2(° C.) and 600 (° C.)≦T2≦850(° C.).

According to an eleventh aspect of the present invention, in the method of manufacturing an epitaxial substrate for semiconductor device according to the ninth or tenth aspect, atmosphere gas other than source gas is nitrogen gas in the barrier layer forming step.

According to a twelfth aspect of the present invention, the method of manufacturing an epitaxial substrate for semiconductor device according to any one of the ninth to eleventh aspects further includes a spacer layer forming step of forming, after the formation of the channel layer, a spacer layer formed of a third group III nitride having a composition of In_(x3)Al_(y3)Ga_(z3)N (x3+y3+z3=1) on the channel layer, the third group III nitride containing at least Al and having larger bandgap energy compared with the barrier layer, wherein the barrier layer is formed on the spacer layer.

According to a thirteenth aspect of the present invention, in the method of manufacturing an epitaxial substrate for semiconductor device according to the twelfth aspect, a temperature T3(° C.) for forming the spacer layer in the spacer layer forming step is substantially equal to the temperature T1(° C.) for forming the channel layer.

According to a fourteenth aspect of the present invention, in the method of manufacturing an epitaxial substrate for semiconductor device according to any one of the ninth to thirteenth aspects, a pressure in a reactor is set to 1 kPa or more and 30 kPa or less in the barrier layer forming step.

According to a fifteenth aspect of the present invention, in the method of manufacturing an epitaxial substrate for semiconductor device according to the fourteenth aspect, the pressure in the reactor is set to 1 kPa or more and 20 kPa or less in the barrier layer forming step.

According to a sixteenth aspect of the present invention, in the method of manufacturing an epitaxial substrate for semiconductor device according to any one of the ninth to fifteenth aspects, a V/III ratio is set to 5,000 or more and 20,000 or less in the barrier layer forming step.

According to the first to sixteenth aspects of the present invention, there are achieved an epitaxial substrate capable of manufacturing a semiconductor device and the semiconductor device, the semiconductor device having a small internal stress due to strains and generating two-dimensional electron gas at concentration of 2×10¹³/cm² or more that is higher than conventional one.

Further, according to the second aspect of the present invention, there are achieved an epitaxial substrate capable of manufacturing a semiconductor device and the semiconductor device, the semiconductor device having a small internal stress due to strains and generating two-dimensional electron gas at higher concentration of 3×10¹³/cm² more.

Further, according to the third, sixth, seventh, twelfth and thirteenth aspects of the present invention, there are achieved an epitaxial substrate capable of manufacturing a semiconductor device and the semiconductor device, the semiconductor device generating two-dimensional electron gas at high concentration and having high mobility.

In particular, according to the thirteenth aspect of the present invention, the temperature is decreased to the bather layer forming temperature after the formation of the spacer layer. Accordingly, the surface of the channel layer is prevented from becoming deteriorated due to temperature drop with the channel layer remaining exposed, which occurs in a case where the spacer layer is not provided.

Further, according to the fourth aspect of the present invention, there are achieved an epitaxial substrate capable of manufacturing a semiconductor device and the semiconductor device, the semiconductor device having high mobility and having a small drain leakage current during OFF.

Further, according to the fifth aspect of the present invention, there are achieved an epitaxial substrate capable of manufacturing a semiconductor device and the semiconductor device, the semiconductor device having a small drain leakage current during OFF and having a high breakdown voltage.

Further, according to the tenth aspect of the present invention, by determining the barrier layer forming temperature in accordance with a target composition of the barrier layer, the barrier layer having the above-mentioned target composition can be formed without fail.

BRIEF DESCRIPTION OF DRAWINGS

FIG. 1 is a schematic cross-sectional view schematically showing a configuration of a HEMT device 10 according to a first embodiment;

FIGS. 2A, 2B, 2C, and 2D are a diagram in which the results obtained by measuring a two-dimensional electron gas concentration are plotted with respect to an InN molar fraction x2 of a barrier layer 5;

FIG. 3 is a diagram in which the relationship between a two-dimensional electron gas concentration and a composition of the barrier layer 5 is mapped on a ternary phase diagram with three components of InN, AlN and GaN being vertices based on the results of FIG. 2A;

FIG. 4 is a diagram in which the relationship between a two-dimensional electron gas concentration and a composition of the barrier layer 5 is mapped on a ternary phase diagram with three components of InN, AlN and GaN being vertices based on the results of FIG. 2B;

FIG. 5 is a diagram in which the relationship between a two-dimensional electron gas concentration and a composition of the barrier layer 5 is mapped on a ternary phase diagram with three components of InN, AlN and GaN being vertices based on the results of FIG. 2C;

FIG. 6 is a diagram in which the relationship between a two-dimensional electron gas concentration and a composition of the barrier layer 5 is mapped on a ternary phase diagram with three components of InN, AlN and GaN being vertices based on the results of FIG. 2D;

FIG. 7 is a diagram for describing how to determine a temperature range of a barrier layer forming temperature T2;

FIG. 8 is a schematic cross-sectional view schematically showing a configuration of a HEMT device 20 according to a second embodiment;

FIG. 9 is a figure showing, as an example, mobilities of the HEMT devices 20 having different compositions of a channel layer 3, a spacer layer 4 and a barrier layer 5;

FIG. 10 is a figure showing, as an example, the relationship between a film thickness of the spacer layer 4 and the mobility of the HEMT device 20;

FIG. 11 is a figure showing a list of measurement results of various characteristics of the HEMT devices 20 having different compositions of the channel layer 3 and the barrier layer 5;

FIG. 12 is a figure showing a list of two-dimensional electron gas concentrations of HEMT devices having different atmospheres for forming a barrier layer;

FIG. 13 is a figure showing a list of pressures in reactor when the barrier layer is formed and various characteristics of manufactured HEMT devices;

FIG. 14 is a figure showing a list of V/III ratios when the barrier layer is formed and various characteristics of manufactured HEMT devices.

BEST MODES FOR CARRYING OUT THE INVENTION First Embodiment Configuration of HEMT Device

FIG. 1 is a schematic cross-sectional view schematically showing the configuration of a HEMT device 10 according to a first embodiment of the present invention. The HEMT device 10 has the configuration in which a substrate 1, a buffer layer 2, a channel layer 3 and a barrier layer 5 are faulted by lamination. The buffer layer 2, the channel layer 3 and the barrier layer 5 are preferred examples of layers that are epitaxially formed (details thereof are described below) using the metal organic chemical vapor deposition method (MOCVD method). Hereinbelow, the laminated structure faulted by laminating the substrate 1, the buffer layer 2, the channel layer 3 and the barrier layer 5 is also referred to as an epitaxial substrate 10A. Note that ratios of respective layers in FIG. 1 do not reflect actual ones.

Hereinbelow, while description is given of a case where the MOCVD method is used for the formation of each layer, other epitaxial growth technique, for example, the method appropriately selected from various vapor phase growth methods and liquid phase growth methods such as MBE, HVPE and LPE may be used, as long as it is the technique capable of forming each layer for providing excellent crystallinity. Alternatively, different growth methods may be used in combination.

Any substrate may be used as the substrate 1 as long as a nitride semiconductor layer having excellent crystallinity can be formed thereon, without any particular limitation. A 6H—SiC single crystal substrate is preferably used as an example, and a substrate composed of sapphire, Si, GaAs, spinel, MgO, ZnO, ferrite or the like may be used.

The buffer layer 2 is formed of AlN to have a thickness of approximately several hundreds of nm, for making crystal quality of the channel layer 3 and the barrier layer 5 that are formed thereon excellent. For example, the buffer layer 2 is preferably formed to have a thickness of 200 nm.

The channel layer 3 is formed of a group III nitride having a composition of In_(x1)Al_(y1)Ga_(z1)N (x1+y1+z1=1) so as to have a thickness of approximately several μm. In this embodiment, the channel layer 3 is formed so as to satisfy a composition range of x1=0 and 0≦y1≦0.3. In the case where 0.3<y1≦1, the cristallinity of the channel layer 3 itself deteriorates remarkably, which makes it difficult to obtain the epitaxial substrate 10A and besides, the HEMT device 10 having excellent electrical characteristics.

On the other hand, the barrier layer 5 is formed of a group III nitride having a composition of In_(x2)Al_(y2)Ga_(z2)N (where x2+y2+z2=1) so as to have a thickness of several nm to several tens of nm.

In the HEMT device 10, a source electrode 6, a drain electrode 7 and a gate electrode 8 are further provided on the barrier layer 5. The source electrode 6 and the drain electrode 7 are multi-layer metal electrodes formed of Ti/Al/Ni/Au each having thickness of approximately ten and several nm to hundred and several tens of nm. The source electrode 6 and the drain electrode 7 have ohmic contact with the barrier layer 5. On the other hand, the gate electrode 8 is a multi-layer metal electrode formed of Pd/Au each having thickness of approximately ten and several nm to hundred and several tens of nm. The gate electrode 8 has schottky contact with the barrier layer 5. Note that the metal used for the source electrode 6 and the drain electrode 7 is not limited to the multi-layer metal formed of Ti/Al/Ni/Au as long as excellent ohmic contact can be obtained with respect to the semiconductor epitaxial substrate according to the present invention and, for example, Ti/Al/Pt/Au or Ti/Al can be used. Similarly, the metal used for the gate electrode 8 is not limited to Pd/Au as long as excellent schottky contact can be obtained with respect to the semiconductor epitaxial substrate according to the present invention and, for example, Pd/Ti/Au or Ni/Au can be used.

In the HEMT device 10 having the above-mentioned layer configuration (in the epitaxial substrate 10A), an interface between the channel layer 3 and the barrier layer 5 becomes a heterojunction interface, and thus a two-dimensional electron gas region 3 e in which two-dimensional electron gas is present at high concentration is formed at the interface (more specifically, at the portion of the channel layer 3 in the vicinity of the interface) by the spontaneous polarization effect and piezo polarization effect. Note that in order to generate the two-dimensional electron gas, the formation is made such that the interface has the mean roughness within a range of 0.1 nm to 3 nm and a surface of the barrier layer 5 for forming this has the mean square roughness within a range of 0.1 nm to 3 nm. Note that a flat interface may be formed exceeding the above-mentioned range, which is not practical considering cost and manufacturing yield. Preferably, the formation is made such that has the mean roughness is within a range of 0.1 nm to 1 nm and the mean square roughness of the surface of the barrier layer 5 in a field of view of 5 μm×5 μm is within a range 0.1 nm to 1 nm. In such a case, more excellent ohmic characteristics are obtained between the source electrode 6 or the drain electrode 7 and the barrier layer 5, and more excellent schottky characteristics are obtained between the gate electrode 8 and the barrier layer 5. Moreover, the effect of confining two-dimensional electron gas is enhanced further, whereby two-dimensional electron gas having higher concentration is generated.

In this embodiment, when the compositions of the group III nitride constituting the channel layer 3 and the barrier layer 5 are caused to satisfy a predetermined requirement, there can be achieved the HEMT device 10 that includes the two-dimensional electron gas region 3 e in which two-dimensional electron gas is present at a higher concentration compared with a conventional case and whose internal stress due to strains has been suppressed. Specifically, two-dimensional electron gas concentration of 2×10¹³/cm² or more is achieved, which is described below in detail. Note that the mobility of two-dimensional electron gas in the HEMT device 10 is approximately 300 to 400 cm²/Vs.

(Relationship Between Composition of Channel Layer and Barrier Layer and Two-Dimensional Electron Gas Concentration)

FIG. 2A to FIG. 2D are diagrams in which the results obtained by measuring a two-dimensional electron gas concentration (2DEG concentration) of a plurality of HEMT devices 10, which were manufactured by fixing the composition of the cannel layer 3 and changing the composition of the barrier layer 5, are plotted with respect to an InN molar fraction x2 of the barrier layer 5. Note that in this specification, the two-dimensional electron gas concentration is measured by the Hall effect method. The compositions of the channel layer 3 corresponding to the respective diagrams are as follows:

FIG. 2A: GaN (x1=y1=0, z1=1);

FIG. 2B: Al_(0.1)Ga_(0.9)N (x1=0, y1=0.1, z1=0.9);

FIG. 2C: Al_(0.2)Ga_(0.8)N (x1=0, y1=0.2, z1=0.8); and

FIG. 2D: Al_(0.3)Ga_(0.7)N (x1=0, y1=0.3, z1=0.7).

FIG. 2A to FIG. 2D suggest the presence of the composition range capable of obtaining a two-dimensional electron gas concentration having an excellent value of 2×10¹³/cm² or more. In addition, the relationship of the respective diagrams suggests that those composition ranges change in accordance with the composition of the channel layer 3.

FIG. 3, FIG. 4, FIG. 5 and FIG. 6 are diagrams, for clarifying the composition ranges, in which the relationship between the two-dimensional electron gas concentration and the composition of the barrier layer 5 is mapped on a ternary phase diagram with three components of InN, AlN and GaN being vertices based on the results of FIG. 2A to FIG. 2D. Note that for the sake of simplification of the diagrams, in FIG. 3 to FIG. 6, mapping of data that does not affect specification of the composition range is omitted. The compositions of the channel layer 3 corresponding to the respective diagrams are as follows:

FIG. 3: GaN (x1=y1=0, z1=1);

FIG. 4: Al_(0.1)Ga_(0.9)N (x1=0, y1=0.1, z1=0.9);

FIG. 5: Al_(0.2)Ga_(0.8)N (x1=0, y1=0.2, z1=0.8); and

FIG. 6: Al_(0.3)Ga_(0.7)N (x1=0, y1=0.3, z1=0.7).

Mapping results shown in FIG. 3 to FIG. 6 lead to a fact that the two-dimensional electron gas concentration in the two-dimensional electron gas region 3 e is equal to or more than 2×10′3/cm² when the barrier layer 5 selects the composition in the range surrounded by five straight lines represented by the expressions described below in the ternary phase diagrams.

$\begin{matrix} \left\lbrack {{Formula}\mspace{14mu} 16} \right\rbrack & \; \\ {{x\; 2} = {\frac{{y\; 2} - \left( {0.36 + {0.5y\; 1}} \right)}{1.78} = {- \frac{{z\; 2} - \left( {0.64 - {0.5y\; 1}} \right)}{2.78}}}} & (1) \\ \left\lbrack {{Formula}\mspace{14mu} 17} \right\rbrack & \; \\ {{x\; 2} = {\frac{{y\; 2} - \left( {0.45 + {y\; 1}} \right)}{4.5} = {- \frac{{z\; 2} - \left( {0.55 - {y\; 1}} \right)}{5.5}}}} & (2) \\ \left\lbrack {{Formula}\mspace{14mu} 18} \right\rbrack & \; \\ {{x\; 2} = {{- \frac{{y\; 2} - \left( {0.9 - {0.7y\; 1}} \right)}{4.5}} = \frac{{z\; 2} - \left( {0.1 + {0.7y\; 1}} \right)}{3.5}}} & (3) \\ \left\lbrack {{Formula}\mspace{14mu} 19} \right\rbrack & \; \\ {{z\; 2} = 0} & (4) \\ \left\lbrack {{Formula}\mspace{14mu} 20} \right\rbrack & \; \\ {{x\; 2} = {0\mspace{14mu} \left( {{{where}\mspace{14mu} \frac{9}{34}} \leq {y\; 1} \leq 0.3} \right)}} & (5) \end{matrix}$

Expressions (1), (2) and (3) include the composition of the channel layer 3 (specifically, value of y1 when x1=0) as a variable, which means that the composition of the barrier layer 5 in which a high two-dimensional electron gas concentration of 2×10¹³/cm² or more is achieved is determined in accordance with the composition of the channel layer 3. Note that in a case where y1<9/34, the confined region is formed by the straight lines represented by Expressions (1) to (4), and thus the straight line represented by Expression (5) is not relevant to defining of the composition range.

On the other hand, as to the epitaxial substrate 10A that was manufactured so as to satisfy the above-mentioned composition range, it has been confirmed from the results of X-ray diffraction measurement that the strains of the barrier layer 5 in an in-plane direction are 1% or less.

The above indicates that, in the HEMT device 10 in which the channel layer 3 and the barrier layer 5 are faulted with the composition satisfying the above-mentioned composition range, the strains due to internal stress are suppressed and the two-dimensional electron gas region 3 e having a concentration of 2×10¹³/cm² or more that is higher compared with a conventional case is formed at the interface between both layers.

Further, the mapping results shown in FIG. 3 to FIG. 6 lead to a fact that the two-dimensional electron gas concentration in the two-dimensional electron gas region 3 e is 3×10¹³/cm² or more when the barrier layer 5 has the composition in the range surrounded by five straight lines represented by expressions described below in a ternary phase diagram.

$\begin{matrix} \left\lbrack {{Formula}\mspace{14mu} 21} \right\rbrack & \; \\ {{x\; 2} = {\frac{{y\; 2} - \left( {0.5 + {0.5y\; 1}} \right)}{1.78} = {- \frac{{z\; 2} - \left( {0.5 - {0.5y\; 1}} \right)}{2.78}}}} & (6) \\ \left\lbrack {{Formula}\mspace{14mu} 22} \right\rbrack & \; \\ {{x\; 2} = {\frac{{y\; 2} - \left( {0.45 + {y\; 1}} \right)}{4.5} = {- \frac{{z\; 2} - \left( {0.55 - {y\; 1}} \right)}{5.5}}}} & (7) \\ \left\lbrack {{Formula}\mspace{14mu} 23} \right\rbrack & \; \\ {{x\; 2} = {{- \frac{{y\; 2} - \left( {0.9 - {0.7y\; 1}} \right)}{4.5}} = \frac{{z\; 2} - \left( {0.1 + {0.7y\; 1}} \right)}{3.5}}} & (8) \\ \left\lbrack {{Formula}\mspace{14mu} 24} \right\rbrack & \; \\ {{z\; 2} = 0} & (9) \\ \left\lbrack {{Formula}\mspace{14mu} 25} \right\rbrack & \; \\ {{x\; 2} = {0\mspace{14mu} \left( {{{where}\mspace{14mu} \frac{9}{34}} \leq {y\; 1} \leq 0.3} \right)}} & (10) \end{matrix}$

Note that in the case where y1<9/34, the confined region is formed by the straight lines represented by Expressions (6) to (9), and thus the straight line represented by Expression (10) is not relevant to defining of the composition range.

The above indicates that, in the HEMT device 10 in which the channel layer 3 and the barrier layer 5 are formed with the composition satisfying the above-mentioned composition range, the two-dimensional electron gas region 3 e having a concentration of 3×10¹³/cm² or more that is higher compared with a conventional case is formed at the interface between both layers.

Note that the discussion regarding the above-mentioned composition range does not exclude a fact that the channel layer 3 and the barrier layer 5 contain impurities. For example, the channel layer 3 and the barrier layer 5 may contain oxygen atoms in the concentration range of 0.0005 at % (1×10¹⁷/cm³) or more to 0.05 at % (1×10¹⁹/cm³) or less, or may contain carbon atoms in the concentration range of 0.0010 at % (2×10¹⁷/cm³) or more to 0.05 at % (1×10¹⁹/cm³) or less. Note that the concentrations of oxygen atoms and carbon atoms may be smaller than respective lower limits of the above-mentioned ranges, which is not practical considering cost and manufacturing yield. On the other hand, when the concentrations of oxygen atoms and carbon atoms exceed respective upper limits of the above-mentioned ranges, the cristallinity of each layer deteriorates to such an extent that device characteristics deteriorate, which is not desirable.

(Relationship Between Composition of Channel Layer and Device Characteristics)

As described above, the channel layer 3 is fowled so as to satisfy the composition range where x1=0 and 0≦y1≦0.3, and in a case where the channel layer 3 is formed so as to satisfy the composition range where x1=0 and 0.01≦y1≦0.1, there is achieved a HEMT device in which the mobility of two-dimensional electron gas is high and the drain leakage current during OFF is small. On the other hand, in a case where the channel layer 3 is faulted so as to satisfy the composition range where x1=0 and 0.1≦y1≦0.3, there is achieved a HEMT device having a small drain leakage current during OFF and a high breakdown voltage. This is specifically described in the second embodiment in which higher mobility is achieved.

(Manufacturing Method for Epitaxial Substrate and HEMT Device)

Next, description is given of the method of manufacturing the epitaxial substrate 10A in which the above-mentioned channel layer 3 and barrier layer 5 have the above-mentioned composition ranges and further manufacturing the HEMT device 10 using the epitaxial substrate 10A.

Note that the case where a large number of HEMT devices 10 are manufactured at the same time from one substrate 1 (in a case where a large number of pieces are manufactured) is described below.

The epitaxial substrate 10A can be manufactured with a known MOCVD apparatus. Specifically, there is used an MOCVD apparatus configured such that a reactor is capable of being supplied with a metal organic (MO) source gas (TMI, TMA and TMG) for In, Al and Ga, an ammonia gas, a hydrogen gas and a nitrogen gas.

First, for example, a 6H—SiC substrate that has (0001) plane orientation and a diameter of two inches is prepared as the substrate 1, and the substrate 1 is placed on a susceptor provided in the reactor of the MOCVD apparatus. The inside of the reactor is vacuumed, and then, an atmosphere in hydrogen/nitrogen mixed flow state is formed while maintaining a pressure inside the reactor at a predetermined value of 5 kPa to 50 kPa (for example, 30 kPa). After that, the temperature of the substrate is raised through susceptor heating.

When the susceptor temperature reaches a predetermined temperature of 950° C. to 1,250° C. (for example, 1,050° C.), which is a buffer layer forming temperature, Al source gas and NH₃ gas are introduced into the reactor, to thereby form an AlN layer serving as the buffer layer 2.

After the AlN layer is formed, the susceptor temperature is maintained at a predetermined channel layer farming temperature T1 (° C.), and metal organic source gas and ammonia gas are introduced into the reactor in accordance with the composition of the channel layer 3, thereby forming an In_(x1)Al_(y1)Ga_(z1)N layer (where x1=0, 0≦y1≦0.3) serving as the channel layer 3. Here, the channel layer forming temperature T1 is a value determined in the temperature range where 950° C.≦T1≦1,250° C. in accordance with a value of an AlN molar fraction y1 of the channel layer 3. Note that the pressure in reactor when forming the channel layer 3 is not particularly limited, and can be appropriately selected from the range of 10 kPa to an atmospheric pressure (100 kPa).

After the In_(x1)Al_(y1)Ga_(z1)N layer is formed, next, the susceptor temperature is maintained at a predetermined barrier layer forming temperature T2(° C.), and then a nitrogen gas atmosphere is formed in the reactor. On that occasion, the pressure in the reactor is maintained at a predetermined value of 1 kPa to 30 kPa (for example, 10 kPa). Note that in the case where the pressure in the reactor is set to a predetermined value of 1 kPa to 20 kPa, the HEMT device 10 that has a small ohmic contact resistance and a small gate leakage current (excellent schottky contact characteristics) is achieved. This is the effect resulting from the increased surface flatness of the barrier layer 5 owing to a reduced reactor pressure.

Next, ammonia gas and metal organic source gas that has a flow rate corresponding to the composition of the barrier layer 5 are introduced into the reactor such that a so-called V/III ratio takes a predetermined value of 3,000 or more and 20,000 or less, and then the In_(x2)Al_(y2)Ga_(z2)N layer serving as the barrier layer 5 is formed to have a predetermined thickness. The In_(x2)Al_(y2)Ga_(z2)N layer is formed so as to have the composition that satisfies Expression (1) to Expression (5). Note that the range of the growth rate of the barrier layer 5 is preferably 0.01 to 0.1 μm/h.

Note that in the case where the V/III ratio is a predetermined value in the range of 3,000 or more to 7,500 or less, the formation is made such that the interface between the channel layer 3 and the barrier layer 5 has the mean roughness in the range of 0.1 nm to 1 nm and the surface of the barrier layer 5 has the mean square roughness in the range of 0.1 nm to 1 nm in a field of view of 5 μm×5 μm.

Here, the barrier layer forming temperature T2(° C.) is determined in a range of 650° C. or more to 800° C. or less and in a temperature range of 800-667·x2(° C.)≦T2≦860-667·x2(° C.) that is determined in accordance with the InN molar fraction x2 of the barrier layer 5.

FIG. 7 is a figure for describing that the barrier layer forming temperature T2 is determined in the above-mentioned temperature range. That is, FIG. 7 is a figure in which InN molar fractions x2 of the barrier layer 5 are plotted with respect to the susceptor temperature in a case where a ratio of a flow amount of In source gas (hereinbelow, In flow rate) to a flow amount of the entire metal organic source gas is changed in a range of 0.5 or more to 0.8 or less and the susceptor temperature in forming a barrier layer (equivalent to the barrier layer forming temperature T2) is changed. Note that the V/III ratio is 5,000.

FIG. 7 reveals that data points are positioned on substantially the same straight line irrespective of the In flow rate. This indicates that the relationship of linear function is substantially established between the barrier layer forming temperature T2 and the InN molar fraction x2. There is no dependence on the InN flow rate, and thus according to the above-mentioned functional relationship, it is concluded that the InN molar fraction of the barrier layer can be controlled by the bather layer forming temperature T2 (susceptor temperature). That is, it is possible to form the barrier layer 5 having an aimed composition.

Specifically, from an arrangement state of the data points in FIG. 7, a regression line represented by the equation T2=830-667·x2 is derived. Therefore, in principle, the barrier layer forming temperature T2 can be determined from the equation above when a desired InN molar fraction x2 is determined. Even in consideration of variations generated by a difference between solid bodies of an MOCVD apparatus or a heating member used in heating, the barrier layer 5 having a desired InN molar fraction x2 can be formed without fail by selecting a preferred temperature in a range of ±30° C. from the equation above. That is, when the relationship of 800-667·x2(° C.)≦T2≦860-667·x2(° C.) is satisfied, the barrier layer 5 can be formed so as to have excellent controllability in a wide composition range, for example, in the composition range determined by Expression (1) to Expression (5) above.

Further, in this embodiment, nitrogen gas is used for bubbling gas of metal organic source and carrier gas in manufacturing the barrier layer 5. That is, the atmosphere gas other than source gas is only nitrogen gas. Accordingly, the hydrogen-terminated dangling bond can be made nitrogen-terminated, and an electron structure of the barrier layer 5 can be maintained in an ideal state, with the result that the generation of two-dimensional electron gas is achieved at high concentration in the two-dimensional electron gas region 3 e. Note that it is not preferable to intentionally mix hydrogen gas into the atmosphere in manufacturing the barrier layer 5 because this causes a decrease in concentration of two-dimensional electron gas.

Manufacturing of the epitaxial substrate 10A is completed after the formation of the barrier layer 5.

After the epitaxial substrate 10A is obtained, the HEMT device 10 is manufactured using this. Note that the steps thereafter are achieved by a known technique.

First, the device isolation step of removing portions that become boundaries between respective devices by etching is performed so as to have a depth of approximately 400 nm by the photolithography process and the RIE method. This device isolation step is required for obtaining a large number of HEMT devices 10 from one epitaxial substrate 10A, which is not necessary for the present invention inherently.

After the device isolation step is performed, an SiO₂ film is formed on the epitaxial substrate 10A to have a predetermined thickness (for example, 10 nm), and then by the photolithography process, the SiO₂ film only in the positions where the source electrode 6 and the drain electrode 7 are to be formed is removed by etching, thereby forming an SiO₂ pattern layer.

After the formation of the SiO₂ pattern layer, the source electrode 6 and the drain electrode 7 formed of Ti/Al/Ni/Au are respectively farmed in the expected formation positions thereof by the vacuum deposition method and the photolithography process. Then, in order to obtain excellent ohmic characteristics of the source electrode 6 and the drain electrode 7, heat treatment is performed for several tens of seconds (for example, 30 seconds) in the nitrogen gas atmosphere at a predetermined temperature of 650° C. to 1,000° C. (for example, 850° C.).

After the heat treatment, the SiO₂ film in the position where the gate electrode 8 is to be formed is removed from the SiO₂ pattern layer by the photolithography process, and then the gate electrode 8 formed of Pd/Au is formed in the expected formation position by the vacuum deposition method and the photolithography process. The gate electrode 8 is formed as a schottky metal pattern.

The HEMT device 10 is obtained by removing the left SiO₂ pattern layer through the photolithography process.

As described above, according to this embodiment, the channel layer is formed so as to satisfy the composition range of In_(x1)Al_(y1)Ga_(z1)N (where x1+y1+z1=1, x1=0, 0≦y1≦0.3), and the epitaxial substrate is manufactured by determining the composition of the barrier layer so as to satisfy the composition range determined by Expression (1) to Expression (5), whereby with the use of this, there is achieved a HEMT device that has strains suppressed due to the internal stress and includes a two-dimensional electron gas region having a concentration of 2×10¹³/cm² or more, which is higher compared with a conventional case. In particular, in the case where an epitaxial substrate is manufactured by determining a composition of a barrier layer so as to satisfy the composition range determined by Expression (6) to Expression (10), there is achieved a HEMT device in which a two-dimensional electron gas region having a concentration of 3×10¹³/cm² or more is formed. Further, the barrier layer that satisfies the above-mentioned composition range is formed under the nitrogen gas atmosphere by preferably determining a pressure and a VIII ratio and setting the forming temperature to a value in a predetermined range corresponding to a molar fraction of InN.

Second Embodiment HEMT Device Including Spacer Layer

FIG. 8 is a schematic cross-sectional diagram schematically showing the configuration of a HEMT device 20 according to a second embodiment of the present invention. The HEMT device 20 has the configuration in which a spacer layer 4 is interposed between the channel layer 3 and the barrier layer 5 of the HEMT device 10 according to the first embodiment. Constituent elements other than the spacer layer 4 are the same as those of the HEMT device 10 according to the first embodiment, and thus detailed description thereof is omitted. Note that the laminated structure in which the substrate 1, the buffer layer 2, the channel layer 3, the spacer layer 4 and the barrier layer 5 are formed by lamination is also referred to as an epitaxial substrate 20A.

The spacer layer 4 is formed of a group III nitride that has a composition of In_(x3)Al_(y3)Ga_(z3)N (x3+y3+z3=1), contains at least Al, and has a bandgap equal to or larger than the bandgap of the barrier layer 5 so as to have a thickness in a range of 0.5 nm to 1.5 nm. For example, in a case where the spacer layer 4 is fondled such that x3=0 and 0≦z3≦0.2, the spacer layer 4 that has a bandgap larger than any barrier layer 5 is formed. The spacer layer 4 is preferably formed such that x3=0 and 0≦z3≦0.05. In such a case, an alloy scattering effect is suppressed, and the concentration and mobility of two-dimensional electron gas are improved. The spacer layer 4 is more preferably formed of AlN (x3=0, y3=1, z3=0). In such a case, the spacer layer 4 is a binary compound of Al and N, and thus an alloy scattering effect is suppressed further compared with the case of a ternary compound containing Ga, with the result that the concentration and mobility of two-dimensional electron gas are improved.

Note that the discussion regarding the above-mentioned composition range does not exclude the fact that the spacer layer 4 contains impurities. For example, in the case where the channel layer 3 contains oxygen atoms or nitrogen atoms in the concentration range as described above, the spacer layer 4 may contain those in a similar concentration range as well.

As described above, in the HEMT device 20 including the spacer layer 4, the two-dimensional electron gas region 3 e in which two-dimensional electron gas is present at high concentration is formed at the interface between the channel layer 3 and the spacer layer 4 (more specifically, in the portion of the channel layer 3 in the vicinity of the interface). If the composition ranges of the channel layer 3 and the barrier layer 5 of the HEMT device 20 are determined in the same manner as the HEMT device 10 according to the first embodiment, two-dimensional electron gas equal to that of the HEMT device 10 having the corresponding composition is generated also in the two-dimensional electron gas region 3 e of the HEMT device 20.

Further, in the HEMT device 20 including the above-mentioned spacer layer 4, the mobility higher than that of the HEMT device 10 according to the first embodiment is achieved. FIG. 9 is a figure showing, as an example, mobilities of the HEMT devices 20 having different compositions of the channel layer 3, the spacer layer 4 and the barrier layer 5. Note that the thickness of each of the spacer layers 4 is 1 nm. In the HEMT device 20, including the case shown in FIG. 9, the mobility of approximately 1,000 to 1,400 cm²/Vs, which is three times or more larger than that of the HEMT device 10, is achieved.

FIG. 10 is a figure showing, as an example, the relationship between the film thickness of the spacer layer 4 and the mobility of the HEMT device 20. Note that a case where the film thickness of the spacer layer 4 is zero is equivalent to the case where the spacer layer is not provided, that is, the first embodiment. FIG. 10 reveals that high mobility is obtained in the case where the spacer layer 4 is formed to have a thickness of 0.5 nm to 1.5 nm as described above. It is considered that in a case where the spacer layer 4 is formed to have a thickness less than 0.5 nm, the layer is insufficiently formed and an effect of confining two-dimensional electron gas is not sufficiently obtained, and that in a case where the spacer layer 4 is formed to have a thickness larger than 1.5 nm, the film quality of the spacer layer 4 itself becomes deteriorated due to an internal stress.

Further, FIG. 11 is a figure showing a list of results obtained by measuring the mobility of two-dimensional electron gas, a full widths at half maximum of peaks of a (0002) plane and a (10-12) plane in an X-ray diffraction profile, a specific resistance of the channel layer 3, a drain leakage current and an off-state breakdown voltage of the HEMT devices 20 in which the compositions of the channel layer 3 and the barrier layer 5 are changed and the spacer layer 4 is formed of AlN to have a thickness of 1 nm.

As can be seen from FIG. 11, in a case where the channel layer 3 contains even a slight amount of Al (in a case where y1>0), a specific resistance thereof increases abruptly and the drain leakage current during OFF decreases abruptly. For example, compared with the case where y1=0 (in which the channel layer 3 is GaN), the specific resistance increases by approximately two orders and drain leakage current decreases by approximately two orders in a case where y1=0.01 (in which the channel layer 3 is Al_(0.01)Ga_(0.99)N). Moreover, in a case where y1=0.1 (in which the channel layer 3 is A1 _(0.01)Ga_(0.9)N), the specific resistance increases by approximately four orders and the drain leakage current decreases by approximately three orders compared with the case where y1=0.

On the other hand, the mobility of two-dimensional electron gas hardly changes in a range where 0≦y1≦0.1. This is considered to result from the fact that the crystallinity of the channel layer does not deteriorate significantly along with an increase in AlN molar fraction and the fact that the mobility deterioration accompanying alloy diffusion (which occurs in a case of mixed crystal material) does not occur considerably due to a relatively small AlN molar fraction.

The mobility of two-dimensional electron gas starts decreasing in the range where y1>0.1, which changes more gradually compared with the specific resistance and the drain leakage current. On the other hand, the off-state breakdown voltage increases as the value of y1 becomes larger, and in the range where y1>0.1, the off-state breakdown voltage twice as large as the case where y1=0 or a larger off-state breakdown voltage is obtained. This is because the breakdown electric field increases along with an increase in bandgap of the channel layer 3.

From the above, when the channel layer 3 is fanned so as to satisfy the composition range where x1=0 and 0.01≦y1≦0.1, the HEMT device 20 that has high mobility of two-dimensional electron gas and a small drain leakage current during OFF is achieved. On the other hand, when the channel layer 3 is formed so as to satisfy the composition range where x1=0 and 0.1y<1≦0.3, the HEMT device 20 that has a small drain leakage current during OFF and has a high breakdown voltage is achieved. Note that the above similarly holds true for the HEMT device 10 that does not include the spacer layer 4 as described above. This is because the respective characteristics shown in FIG. 11 do not depend on the presence/absence of the spacer layer 4 except for the mobility.

(Manufacture of HEMT Device Including Spacer Layer)

The HEMT device 20 having the above-mentioned structure is manufactured by a similar method to that of the HEMT device 10 according to the first embodiment except for the process of forming the spacer layer 4.

Specifically, in manufacturing the epitaxial substrate 20A, the formation up to the channel layer 3 is performed, the susceptor temperature is set to a spacer layer forming temperature T3 (where T3 is approximately the same as Ti), and the inside of the reactor is maintained at the nitrogen gas atmosphere. After that, the reactor pressure is set to 10 kPa, and then metal organic source gas and ammonia gas are introduced into the reactor, thereby forming the In_(x3)Al_(y3)Ga_(z3)N layer serving as the spacer layer 4 to have a predetermined thickness.

The spacer layer 4 is formed in this manner, and then the barrier layer 5 is manufactured in a similar procedure to that in the case of manufacturing the above-mentioned epitaxial substrate 10A.

Note that the channel layer forming temperature T1 is set in the range where 950° C.≦T1≦1,250° C., whereas the barrier layer forming temperature T2 is set in accordance with the InN molar fraction of the barrier layer 5 in the range where 650° C.<T2≦800° C., as described above. In addition, the spacer layer forming temperature T3(° C.) is set to be approximately the same as the channel layer forming temperature T1(° C.) as well. Therefore, in order to form the barrier layer 5, the susceptor temperature needs to be lowered after the formation of the channel layer 3 or the spacer layer 4. In the course of manufacturing the HEMT device 10 according to the first embodiment, in which the spacer layer 4 is not provided, the surface of the channel layer 3 remains exposed while the temperature drops, and thus this surface may be etched by atmosphere gas. To the contrary, in the case where the spacer layer 4 is provided at the spacer layer forming temperature T3 that is approximately the same as the channel layer forming temperature T1 as in this embodiment, the susceptor temperature is lowered after the formation of the spacer layer 4, whereby the spacer layer 4 acts as a protective layer of the surface of the channel layer 3. It is considered that the above also contributes to improvement in mobility of two-dimensional electron gas.

As described above, according to this embodiment, in a HEMT device in which the compositions of a channel layer and a barrier layer are determined as in the HEMT device according to the first embodiment, by providing a spacer layer between the channel layer and the barrier layer, it is possible to achieve a HEMT device that has improved mobility of two-dimensional electron gas while having a high two-dimensional electron gas concentration similar to that of the HEMT device according to the first embodiment.

EXAMPLES Example 1

In this example, the HEMT device 10 according to the first embodiment was manufactured. Specifically, a plurality of epitaxial substrates 10A having different combinations of the channel layer 3 and the barrier layer 5 were manufactured, to thereby manufacture the HEMT device 10 using each of them.

In manufacturing the epitaxial substrates 10A, first, a plurality of 6H—SiC substrates that have (0001) plane orientation and a diameter of two inches were prepared as the substrate 1. Each of the substrates 1 was placed in a reactor of an MOCVD apparatus, and an inside of the reactor was vacuumed. After that, a pressure inside the reactor was set to 30 kPa, thereby forming the atmosphere in hydrogen/nitrogen mixed flow state. Then, a temperature of the substrate was raised through susceptor heating.

When a susceptor temperature reached 1,050° C., Al source gas and ammonia gas were introduced into the reactor, to thereby form an AlN layer that serves as the buffer layer 2 and has a thickness of 200 nm.

Then, the susceptor temperature was maintained at a predetermined channel layer forming temperature T1(° C.) that is determined in a range where 950° C.≦T1≦1,250° C. in accordance with a target composition of the channel layer 3, and metal organic source gas and ammonia gas were introduced into the reactor at a flow rate corresponding to the target composition, to thereby form an In_(x1)Al_(y1)Ga_(z1)N layer serving as the channel layer 3 to have a thickness of 2 μm. Note that the target composition of the channel layer 3 was set as four patterns in a manner that (x1, y1, z1)=(0, 0, 1), (0, 0.1, 0.9), (0, 0.2, 0.8) and (0, 0.3, 0.7). The channel layer forming temperature T1 thereof was set as 1,080° C., 1,100° C., 1,130° C. and 1,180° C.

After the channel layer 3 was obtained, the susceptor temperature was kept at the barrier layer forming temperature T2(° C.) determined by the equation T2=830-667·x2 in accordance with a target composition of the barrier layer 5, and the reactor pressure was set to 10 kPa after a nitrogen atmosphere was formed in the reactor. Then, metal organic source gas and ammonium gas were introduced into the reactor at the flow rate corresponding to the target composition, whereby an In_(x2)Al_(y2)Ga_(z2)N layer serving as the barrier layer 5 was formed to have a thickness of 15 nm. Note that nitrogen gas was used for bubbling gas of metal organic source and carrier gas. The V/III ratio was set to 5,000.

After the formation of the barrier layer 5, the susceptor temperature was lowered to approximately room temperature. Then, the reactor was made open to the atmosphere after the inside of the reactor was returned to the atmospheric pressure, and then the manufactured epitaxial substrate 10A was taken out.

Next, the HEMT device 10 was manufactured using this epitaxial substrate 10A. Note that the HEMT device was designed such that a gate width was 1 mm, a source-gate distance was 0.5 μm, a gate-drain distance was 7.5 μm, and a gate length was 1.5 μm.

First, the portions that become boundaries between respective devices were removed by etching so as to have a depth of approximately 400 nm by the photolithography process and the RIE method.

Next, an SiO₂ film was formed on the epitaxial substrate 10A to have a thickness of 10 nm, and then by photolithography, the SiO₂ film in the positions where the source electrode 6 and the drain electrode 7 were to be formed was removed by etching, thereby obtaining an SiO₂ pattern layer.

Next, a metal pattern formed of Ti/Al/Ni/Au (film thickness thereof was 25/75/15/100 nm) was formed in the expected formation positions of the source electrode 6 and the drain electrode 7 by the vacuum deposition method and the photolithography process, to thereby form the source electrode 6 and the drain electrode 7. Then, in order to obtain excellent ohmic characteristics of the source electrode 6 and the drain electrode 7, heat treatment was performed for 30 seconds in the nitrogen gas atmosphere at 850° C.

Then, the SiO₂ film in the expected formation position of the gate electrode 8 was removed from the SiO₂ pattern layer using the photolithography process. Further, using the vacuum deposition method and photolithography, the gate electrode 8 was formed as the schottky metal pattern formed of Pd/Au (film thickness thereof was 30/100 nm) in the expected formation position.

Through the process described above, the HEMT device 10 was obtained.

Note that for enabling measurement of the device characteristics, a passivation film of silicon nitride was formed in this HEMT device 10 using the CVD method and photolithography process, and then contact holes were made at positions corresponding to the source electrode 6, drain electrode 7 and gate electrode 8 of the passivation film, whereby wire bonding was performed.

The two-dimensional electron gas concentration and mobility of the plurality of HEMT devices 10 obtained in this manner were measured by the Hall effect method.

FIG. 2A to FIG. 2D show the results obtained by fixing the composition of the channel layer 3 and plotting the two-dimensional electron gas concentration obtained by measurement with respect to the composition (specifically, InN molar fraction) of the barrier layer 5. FIG. 3 to FIG. 6 show the results obtained by plotting pieces of data of FIG. 2A to FIG. 2A (exclusive of part thereof) in a ternary phase diagram with InN, AlN and GaN being vertices. Note that the mobility of two-dimensional electron gas took a value in the range of 300 to 400 cm²/Vs.

The results above confirmed that a HEMT device that generates two-dimensional electron gas at high concentration of 2×10¹³/cm² or more was achieved by forming the channel layer 3 so as to satisfy the composition range of In_(x1)Al_(y1)Ga_(z1)N (where x1+y1+z1=1, x1=0, 0≦y1<0.3) and forming the barrier layer 5 so as to satisfy the composition range surrounded by the straight lines specified by Equation (1) to Equation (5) above in the ternary phase diagram as shown in FIG. 3 to FIG. 6.

On the other hand, the results of X-ray diffraction measurement performed on the epitaxial substrate 10A also confirmed that strains in an in-plane direction fall within 1% in the barrier layer 5 affiliated with the composition range represented by Equation (1) to Equation (5) above in the ternary phase diagram. That is, it was confirmed that strains in the barrier layer were suppressed and a HEMT device having high two-dimensional electron gas concentration was achieved by manufacturing the barrier layer 5 so as to be affiliated with the composition ranges represented by Equations (1) to (5).

Further, it was confirmed that a HEMT device that generates two-dimensional electron gas at high concentration of 3×10¹³/cm² or more was achieved by forming the barrier layer 5 so as to satisfy the composition range surrounded by straight lines specified by Equation (6) to Equation (10) above in a ternary phase diagram.

Comparative Example 1

In this comparative example, the HEMT device was manufactured in a similar procedure to that of Example 1 except for that hydrogen was intentionally mixed into atmosphere gas in forming the barrier layer 5. FIG. 12 is a figure showing a list of two-dimensional electron gas concentrations of the HEMT device obtained in Example 1 and the HEMT device according to this comparative example that was obtained in the atmosphere into which hydrogen was mixed. Note that FIG. 12 shows, as a representative example, the results of two patterns of HEMT devices having different combinations of the composition of the channel layer 3 and the composition of the barrier layer 5. In addition, FIG. 12 shows the technique of mixing hydrogen in this comparative example as well.

As shown in FIG. 12, it was confirmed that the two-dimensional electron gas concentration decreased considerably in the HEMT device in which hydrogen was mixed into atmosphere gas in forming the barrier layer. That is, it was confirmed that the barrier layer was effectively formed in the atmosphere free from hydrogen, for example, in the nitrogen gas atmosphere as in Example 1.

Example 2

In this example, the HEMT device 20 according to the second embodiment was manufactured. Note that a procedure and manufacturing conditions similar to those of Example 1 were used except that the composition of the channel layer 3 was set as six patterns in which two patterns (x1, y1, z1)=(0, 0.01, 0.99), (0, 0.05, 0.95) were added to the four patterns described in Example 1, and that the formation step for the spacer layer 4 was provided between the formation step for the channel layer 3 and the formation step for the barrier layer 5.

Specifically, after the formation of the channel layer 3, the susceptor temperature was kept at the predetermined spacer layer forming temperature T3 and the reactor pressure was set to 10 kPa. After that, metal organic source gas and ammonia gas were introduced into the reactor to form an In_(x3)Al_(y3)Ga_(z3)N layer serving as the spacer layer 4, and then the channel layer 5 was formed. Note that the target composition of the spacer layer 4 was set as two patterns, (x3, y3, z3)=(0, 1, 0) and (0, 0.9, 0.1). The spacer layer forming temperature T3 thereof was made to be the same temperature as the channel layer forming temperature T1. In addition, the thickness of the spacer layer 4 was set as five levels of 0.3 nm, 0.5 nm, 1 nm, 1.5 nm and 2 nm.

As in Example 1, the concentration and mobility of two-dimensional electron gas of the obtained HEMT device 20 were measured and, at the same time, the X-ray diffraction, channel layer specific resistance, drain leakage current and off-state breakdown voltage thereof were measured. Measurement was performed during OFF in the state where −10 V was applied as a gate bias voltage. In addition, as a drain leakage current, a current value when the source-drain voltage was 100 V was measured.

FIG. 9 shows the composition of the spacer layer 4 and the mobility of several HEMT devices 20 having different compositions of the channel layer 3 and the barrier layer 5. FIG. 9 shows the results in a case where the film thicknesses of the spacer layers 4 were each 1 nm. FIG. 10 shows the relationship between the film thickness of the spacer layer 4 and the mobility of two-dimensional electron gas. FIG. 10 shows the results in the case where the AlN layer was formed as the spacer layer 4. Those results reveal that by providing the spacer layer 4 having a thickness in a range of 0.5 nm to 1.5 nm, a HEMT device having a mobility three to four times higher compared with a HEMT device in which this was not provided was obtained. Note that a remarkable difference was not observed in two-dimensional electron gas concentration with the HEMT device according to Example 1 in which the spacer layer 4 was not provided.

Further, FIG. 11 shows mobilities, full widths at half maximum of peaks of a (0002) plane and a (10-12) plane in X-ray diffraction profile, channel layer specific resistances, drain leakage currents and off-state breakdown voltages of several HEMT devices 20 that have different compositions of the channel layer 3 and the barrier layer 5. The results of FIG. 11 confirmed that a HEMT device having high mobility of two-dimensional electron gas and small drain leakage current during OFF was achieved by forming the channel layer 3 so as to satisfy the composition range where x1=0 and 0.01≦y1≦0.1 and that a HEMT device having a small drain leakage current during OFF and a high breakdown voltage was achieved by forming the channel layer 3 so as to satisfy the composition range where x1=0 and 0.1≦y1≦0.3.

Example 3

In this example, a HEMT device was manufactured in a similar procedure to that of Example 2 except for that the pressure in a reactor when forming the barrier layer 5 was changed. The two-dimensional electron gas concentration and mobility of the obtained HEMT device were measured, and further, the measurement of the surface mean square roughness with an AFM, the measurement of contact resistance and the measurement of gate leakage current were performed. FIG. 13 is a figure showing a list of pressures in a reactor and the measurement results of the respective measurements above of the HEMT devices obtained in this example. Note that FIG. 13 shows, as a representative example, the results of two patterns of HEMT devices that have different combinations of the composition of the channel layer 3 and the composition of the barrier layer 5.

It was confirmed from the results shown in FIG. 13 that two-dimensional electron gas having a high concentration and a high mobility is generated by setting the pressure in a reactor when forming the barrier layer 5 to 1 kPa or more and 30 kPa or less. Moreover, it was confirmed that a HEMT device having a low ohmic contact resistance and a small gate leakage current (excellent schottky contact characteristics) is obtained by setting the pressure in a reactor to 1 kPa or more and 20 kPa or less. This is considered to result from the fact that the surface flatness is improved (value of surface mean square roughness becomes smaller) by reducing the pressure in a reactor.

Example 4

In this example, a HEMT device was manufactured in a similar procedure to that of Example 2 except for that a V/III ratio in forming the barrier layer 5 was changed. The two-dimensional electron gas concentration and mobility of the obtained HEMT devices were measured, and further, the measurement of the surface mean square roughness with an AFM, the measurement of contact resistance and the measurement of gate leakage current were performed. FIG. 14 is a figure showing a list of pressures in a reactor and measurement results of the measurements above of the HEMT devices obtained in this example. Note that FIG. 14 shows the results of two patterns of HEMT devices that have different combinations of the composition of the channel layer 3 and the composition of the barrier layer 5.

It was confirmed from the results shown in FIG. 14 that by setting a V/III ratio in forming the barrier layer 5 to 3,000 or more and 20,000 or less, a HEMT device that generates two-dimensional electron gas having high concentration and mobility and has excellent device characteristics is obtained. 

1. An epitaxial substrate for semiconductor device, comprising: a base substrate; a channel layer formed of a first group III nitride containing at least Al and Ga and having a composition of In_(x1)Al_(y1)Ga_(z1)N (x1+y1+z1=1); and a barrier layer formed of a second group III nitride containing at least In and Al and having a composition of In_(x2)Al_(y2)Ga_(z2)N (x2+y2+z2=1), wherein: the composition of said first group III nitride is in a range determined by x1=0 and 0≦y1≦0.3; and the composition of said second group III nitride is, in a ternary phase diagram with InN, AlN and GaN being vertices, in a range surrounded by straight lines respectively represented by the following expressions determined in accordance with the composition of said first group III nitride: $\begin{matrix} {{{x\; 2} = {\frac{{y\; 2} - \left( {0.36 + {0.5y\; 1}} \right)}{1.78} = {- \frac{{z\; 2} - \left( {0.64 - {0.5y\; 1}} \right)}{2.78}}}};} \\ {{{x\; 2} = {\frac{{y\; 2} - \left( {0.45 + {y\; 1}} \right)}{4.5} = {- \frac{{z\; 2} - \left( {0.55 - {y\; 1}} \right)}{5.5}}}};} \\ {{{x\; 2} = {{- \frac{{y\; 2} - \left( {0.9 - {0.7y\; 1}} \right)}{4.5}} = \frac{{z\; 2} - \left( {0.1 + {0.7y\; 1}} \right)}{3.5}}};} \\ {{{z\; 2} = 0};{and}} \\ {{x\; 2} = {0\mspace{14mu} {\left( {{{where}\mspace{14mu} \frac{9}{34}} \leq {y\; 1} \leq 0.3} \right).}}} \end{matrix}$
 2. The epitaxial substrate for semiconductor device according to claim 1, wherein the composition of said second group III nitride is, in a ternary phase diagram with InN, AlN and GaN being vertices, in a range surrounded by straight lines respectively represented by the following expressions: $\begin{matrix} {{{x\; 2} = {\frac{{y\; 2} - \left( {0.5 + {0.5y\; 1}} \right)}{1.78} = {- \frac{{z\; 2} - \left( {0.5 - {0.5y\; 1}} \right)}{2.78}}}};} \\ {{{x\; 2} = {\frac{{y\; 2} - \left( {0.45 + {y\; 1}} \right)}{4.5} = {- \frac{{z\; 2} - \left( {0.55 - {y\; 1}} \right)}{5.5}}}};} \\ {{{x\; 2} = {{- \frac{{y\; 2} - \left( {0.9 - {0.7y\; 1}} \right)}{4.5}} = \frac{{z\; 2} - \left( {0.1 + {0.7y\; 1}} \right)}{3.5}}};} \\ {{{z\; 2} = 0};{and}} \\ {{x\; 2} = {0\mspace{14mu} {\left( {{{where}\mspace{14mu} \frac{9}{34}} \leq {y\; 1} \leq 0.3} \right).}}} \end{matrix}$
 3. The epitaxial substrate for semiconductor device according to claim 1, further comprising: a spacer layer formed of a third group III nitride having a composition of In_(x3)Al_(y3)Ga_(z3)N (x3+y3+z3=1), said spacer layer being formed between said channel layer and said barrier layer, containing at least Al, and having larger bandgap energy compared with said barrier layer.
 4. The epitaxial substrate for semiconductor device according to claim 1, wherein the composition of said first group III nitride is in a range determined by x1=0 and 0<y1≦0.1.
 5. The epitaxial substrate for semiconductor device according to claim 1, wherein the composition of said first group III nitride is in a range determined by x1=0 and 0.1<y1≦0.3.
 6. The epitaxial substrate for semiconductor device according to claim 3, wherein the composition of said third group III nitride is in a range determined by x3=0 and 0≦z3≦0.05.
 7. The epitaxial substrate for semiconductor device according to claim 6, wherein said third group III nitride is AlN.
 8. A semiconductor device, comprising: an epitaxial substrate for semiconductor device, comprising, a base substrate, a channel layer formed of a first group III nitride containing at least Al and Ga and having a composition of In_(x1)Al_(y1)Ga_(z1)N (x1+y1+z1=1), and a barrier layer formed of a second group III nitride containing at least In and Al and having a composition of In_(x2)Al_(y2)Ga_(z2)N (x2+y2+z2=1); and a source electrode, a drain electrode and a gate electrode formed on said barrier layer of the epitaxial substrate for semiconductor device, wherein: the composition of said first group III nitride is in a range determined by x1=0 and 0≦y1≦0.3; and the composition of said second group III nitride is, in a ternary phase diagram with InN, AlN and GaN being vertices, in a range surrounded by straight lines respectively represented by the following expressions determined in accordance with the composition of said first group III nitride: $\begin{matrix} {{{x\; 2} = {\frac{{y\; 2} - \left( {0.36 + {0.5y\; 1}} \right)}{1.78} = {- \frac{{z\; 2} - \left( {0.64 - {0.5y\; 1}} \right)}{2.78}}}};} \\ {{{x\; 2} = {\frac{{y\; 2} - \left( {0.45 + {y\; 1}} \right)}{4.5} = {- \frac{{z\; 2} - \left( {0.55 - {y\; 1}} \right)}{5.5}}}};} \\ {{{x\; 2} = {{- \frac{{y\; 2} - \left( {0.9 - {0.7y\; 1}} \right)}{4.5}} = \frac{{z\; 2} - \left( {0.1 + {0.7y\; 1}} \right)}{3.5}}};} \\ {{{z\; 2} = 0};{and}} \\ {{x\; 2} = {0\mspace{14mu} {\left( {{{where}\mspace{14mu} \frac{9}{34}} \leq {y\; 1} \leq 0.3} \right).}}} \end{matrix}$
 9. A method of manufacturing an epitaxial substrate for semiconductor device, comprising: a channel layer forming step of epitaxially forming a channel layer formed of a first group III nitride on a base substrate, the first group III nitride containing at least Al and Ga and having a composition of In_(x1)Al_(y1)Ga_(z1)N (x1+y1+z1=1); and a barrier layer forming step of epitaxially forming a barrier layer formed of a second group III nitride on said channel layer, the second group III nitride containing at least In and Al and having a composition of In_(x2)Al_(y2)Ga_(z2)N (x2+y2+z2=1), wherein: the composition of said first group III nitride is selected in a range determined by x1=0 and 0≦y1≦0.3; and the composition of said second group III nitride is selected, in a ternary phase diagram with InN, AlN and GaN being vertices, in a range surrounded by straight lines respectively represented by the following expressions determined in accordance with the composition of said first group III nitride: $\begin{matrix} {{{x\; 2} = {\frac{{y\; 2} - \left( {0.36 + {0.5y\; 1}} \right)}{1.78} = {- \frac{{z\; 2} - \left( {0.64 - {0.5y\; 1}} \right)}{2.78}}}};} \\ {{{x\; 2} = {\frac{{y\; 2} - \left( {0.45 + {y\; 1}} \right)}{4.5} = {- \frac{{z\; 2} - \left( {0.55 - {y\; 1}} \right)}{5.5}}}};} \\ {{{x\; 2} = {{- \frac{{y\; 2} - \left( {0.9 - {0.7y\; 1}} \right)}{4.5}} = \frac{{z\; 2} - \left( {0.1 + {0.7y\; 1}} \right)}{3.5}}};} \\ {{{z\; 2} = 0};{and}} \\ {{x\; 2} = {0\mspace{14mu} {\left( {{{where}\mspace{14mu} \frac{9}{34}} \leq {y\; 1} \leq 0.3} \right).}}} \end{matrix}$
 10. The method of manufacturing an epitaxial substrate for semiconductor device according to claim 9, wherein: a temperature T1(° C.) for forming said channel layer is determined in a range where 950° C.≦T1≦1,250° C.; and a temperature T2(° C.) for forming said barrier layer is determined in a range determined in accordance with a molar fraction x2 of InN of said second group III nitride, the range satisfying: 800-667·x2(° C.)≦T2≦860-667-x2(° C.); and 600° C.≦T2≦850° C.
 11. The method of manufacturing an epitaxial substrate for semiconductor device according to claim 9, wherein atmosphere gas other than source gas is nitrogen gas in said barrier layer forming step.
 12. The method of manufacturing an epitaxial substrate for semiconductor device according to claim 9, further comprising: a spacer layer forming step of forming, after the formation of said channel layer, a spacer layer formed of a third group III nitride having a composition of In_(x3)Al_(y3)Ga_(z3)N (x3+y3+z3=1) on said channel layer, said third group III nitride containing at least Al and having larger bandgap energy compared with said barrier layer, wherein said barrier layer is faulted on said spacer layer.
 13. The method of manufacturing an epitaxial substrate for semiconductor device according to claim 12, wherein a temperature T3(° C.) for forming said spacer layer in said spacer layer forming step is substantially equal to said temperature T1(° C.) for forming said channel layer.
 14. The method of manufacturing an epitaxial substrate for semiconductor device according to claim 9, wherein a pressure in a reactor is set to 1 kPa or more and 30 kPa or less in said barrier layer fowling step.
 15. The method of manufacturing an epitaxial substrate for semiconductor device according to claim 14, wherein the pressure in the reactor is set to 1 kPa or more and 20 kPa or less in said barrier layer forming step.
 16. The method of manufacturing an epitaxial substrate for semiconductor device according to claim 9, wherein a V/III ratio is set to 5,000 or more and 20,000 or less in said barrier layer forming step.
 17. The epitaxial substrate for semiconductor device according to claim 2, further comprising: a spacer layer formed of a third group III nitride having a composition of In_(x3)Al_(y3)Ga_(z3)N (x3+y3+z3=1), said spacer layer being formed between said channel layer and said barrier layer, containing at least Al, and having larger bandgap energy compared with said barrier layer.
 18. The epitaxial substrate for semiconductor device according to claim 17, wherein the composition of said third group III nitride is in a range determined by x3=0 and 0≦z3≦0.05.
 19. The epitaxial substrate for semiconductor device according to claim 18, wherein said third group III nitride is AlN.
 20. The method of manufacturing an epitaxial substrate for semiconductor device According to claim 10, further comprising: a spacer layer forming step of limning, after the formation of said channel layer, a spacer layer formed of a third group III nitride having a composition of In_(x3)Al_(y3)Ga_(z3)N (x3+y3+z3=1) on said channel layer, said third group III nitride containing at least Al and having larger bandgap energy compared with said barrier layer, wherein said barrier layer is formed on said spacer layer. 